
A Feynman diagram is a pictorial method for calculating particle interaction probabilities in quantum field theory.Particles at the quantum level constantly transform into each other. A Feynman diagram is a visual scheme where lines are particles and the points where lines meet are moments of their interaction. Like a traffic diagram for the microworld.
Introduced by Richard Feynman in 1948 as an alternative to cumbersome S-matrix calculations. The idea grew out of his work on quantum electrodynamics, where he interpreted positrons as electrons moving backward in time. Later, Julian Schwinger and Sin-Itiro Tomonaga independently developed similar methods, but Feynman's approach became the standard. Feynman, Schwinger, and Tomonaga shared the 1965 Nobel Prize. Over time, diagrams spread to all gauge theories, including quantum chromodynamics and electroweak theory.
In quantum electrodynamics, the electron line is represented by the propagator i(γ^μ p_μ + m)/(p^2 - m^2 + iε), the photon line by -i g_μν/(k^2 + iε). The interaction vertex gives a factor -i e γ^μ. Integration over all internal momenta yields the diagram's contribution to the amplitude. Feynman rules allow automatically accounting for Fermi statistics through diagram signs. The superposition principle and gauge invariance ensure the renormalizability of the theory, where infinities cancel when defining physical parameters.
Feynman himself drew these diagrams on napkins in cafes. Now, no research in particle physics is complete without them.




